Autoranging phase-lock-loop circuit

ABSTRACT

An autoranging phase-lock-loop circuit compares an oscillator signal output from a range programmable voltage controlled oscillator, which generates the oscillator frequency within one of a plurality of operating ranges, to a reference signal and commands the voltage controlled oscillator to step to a next operating range if the voltage controlled oscillator cannot lock onto the reference signal within a prescribed time.

RELATED APPLICATION

The present application is related to commonly-assigned U.S. patent application Ser. No. 07,914,977 filed by Michael Arthur Brown of even date herewith, for A LOW-GAIN, RANGE PROGRAMMABLE, TEMPERATURE COMPENSATED VOLTAGE CONTROLLED OSCILLATOR. The referenced related application is hereby incorporated by reference to provide additional background information regarding the present invention.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a phase-lock-loop for controlling a voltage controlled oscillator and, in particular, to an autoranging phase-lock-loop circuit for controlling a range programmable voltage controlled oscillator.

2. Description of the Related Art

The approach used to control a voltage controlled oscillator (VCO) in a typical phase-lock-loop circuit is a feedback loop that measures a phase error between an input reference signal and a VCO output signal. In the typical approach, the feedback loop modifies a VCO input control voltage to drive the phase and frequency of the VCO output signal to match the phase and frequency of the input reference signal. This results in a one-to-one relationship between the VCO input control voltage and the frequency of the VCO output signal.

One major limitation to this approach is that in order to guarantee the dynamic range of the VCO relative to the input reference signal, the VCO must be designed to operate over a wide range of frequencies (as much as a 10X range of frequencies) to account for variations in the fabrication of the VCO as well as variations in the operating conditions of the circuit such as changes in the supply voltage and ambient temperature.

A second major limitation is that a wide-pull, high-gain VCO is more susceptible to noise and circuit coupling problems than a narrow-pull, low-gain VCO. However, a narrow-pull, low-gain VCO presents problems of its own. For example, the low-gain VCO lacks the dynamic range necessary to guarantee that the VCO will function over all variations in fabrication, temperature, and supply voltage.

One solution to this problem is to design a VCO that has multiple overlapping low-gain frequency ranges such that the loop will have sufficient dynamic range for variations in fabrication, temperature, and supply voltage. Since both supply and temperature conditions are environmentally controlled (continuously varying) and the fabrication variations are fixed (once a device has been manufactured, it does not change), these two variations can be treated differently.

The problem with this solution, however, is that in a typical phase-lock-loop circuit, the feedback loop will be able to match the phase and frequency of the input reference signal in only one low-gain frequency range because there is no mechanism for stepping the VCO from one low-gain frequency range to another to find the optimal VCO frequency range of operation for that specific device (accommodate the fabrication variations).

Several mechanisms for stepping from one low-gain frequency range to another are available, however, each mechanism has drawbacks that make it unacceptable. One approach is to measure the VCO at the factory to determine the optimum range of operation and then provide the information to the end user who must then program the VCO to the proper operating range.

This approach presents several drawbacks. First, current factory testing must be expanded to accommodate measurements of the optimum range with a resulting increase in time and cost. Second, the end user must program the VCO, resulting in additional time and cost to the end user.

Another approach is to design programmable fuses into the VCO. In this approach, the VCO characteristics are measured at the factory and then a testing device programs the VCO as is done with PROM devices. The drawback here is that the fabrication process is necessarily more complicated with lower yields, and resulting higher device production costs.

Thus, there is a need for a mechanism for stepping a multiple-range low-gain VCO from one low-gain frequency range to another which solves the above described problems.

SUMMARY OF THE INVENTION

In accordance with the present invention, a range programmable voltage controlled oscillator in an autoranging phase-lock-loop is disclosed. The range programmable voltage controlled oscillator, which has a plurality of low-gain frequency ranges, generates a current oscillator signal in response to one of a plurality of range select signals and a loop filter voltage. The range select signals select which of the low-gain frequency ranges the range programmable voltage controlled oscillator will operate in. The loop filter voltage varies the frequency of the oscillator signal within each low-gain frequency range. A timer generates a first enable signal a preselected settling time after receiving a reset signal and removes the first enable signal a preselected turn-off time after generating the first enable signal if the timer has not received a subsequent reset signal since the most recent first enable signal was generated. A phase error detector compares the current oscillator signal to a reference signal when the first enable signal is received and generates a shift signal and the reset signal if a phase error is present. The phase error detector stops comparing the current oscillator signal and the reference signal when the first enable signal is removed. A shift register receives the shift signal and then generates a new range select signal. The VCO receives the new range select signal and shifts into a new low-gain frequency range. A phase comparator compares the current oscillator signal to the reference signal and generates a difference signal in response. A loop filter generates the loop filter voltage in response to the difference signal.

A better understanding of the features and advantages of the present invention will be obtained by reference to the following detailed description and accompanying drawings which set forth an illustrative embodiment in which the principles of the invention are utilized.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a block diagram illustrating an autoranging phase-lock-loop circuit in accordance with the present invention.

FIG. 2 is a graphical representation of five oscillator operating ranges as a function of loop filter voltage.

FIG. 3 is a flow chart illustrating the operation of the FIG. 1 autoranging phase-lock-loop circuit.

FIGS. 4A, 4B, 4C, 4D, 4E and 4F are schematic diagrams illustrating a portion of an embodiment of the FIG. 1 autoranging phase-lock-loop circuit.

FIG. 5 is a block diagram illustrating a range programmable voltage controlled oscillator utilizable in the FIG. 1 circuit.

FIG. 6 is a schematic diagram illustrating one oscillator stage of the range programmable voltage controlled oscillator shown in FIG. 5.

FIG. 7 is a schematic diagram illustrating one oscillator stage of the FIG. 5 range programmable voltage controlled oscillator.

FIGS. 8A, 8B, 8C, and 8D are schematic diagrams illustrating a portion of an embodiment of three FIG. 7 oscillator circuits.

FIG. 9 is a schematic diagram illustrating a VGS and VSW generation circuit utilizable in the voltage controlled oscillator shown in FIG. 5.

FIG. 10 is a schematic diagram illustrating an embodiment of three FIG. 9 VGS and VSW generator circuit.

FIG. 11 is a schematic diagram illustrating a temperature compensation circuit utilizable in the voltage controlled oscillator shown in FIG. 5.

FIGS. 12A and 12B are schematic diagrams illustrating a portion of an embodiment of the voltage translator circuit.

FIGS. 12C and 12D are schematic diagrams illustrating a portion of an embodiment of the voltage translator circuit and the FIG. 11 temperature compensation circuit.

DETAILED DESCRIPTION

FIG. 1 shows an autoranging phase-lock-loop circuit 112 that provides a means for locking a divided oscillator output signal OSCD of a voltage controlled oscillator (VCO) 110 to a reference signal REF by increasing ordecreasing the frequency of divided oscillator output signal OSCD until thefrequency of divided oscillator output signal OSCD matches the frequency ofreference signal REF.

Phase-lock-loop circuit 112 includes a range programmable voltage controlled oscillator 110 that generates an oscillator output signal OSC, which has a predicted frequency of 250 MHz, in one of five oscillator ranges in response to one of five corresponding range select signals RSS0-RSS4. In addition, VCO 110 varies the frequency of oscillator output signal OSC in response to a loop filter voltage LFV.

A first divider circuit 130 receives oscillator output signal OSC and generates a divide-by-two oscillator output signal OSC2 which has a predicted frequency of 125 MHz. A second divider circuit 132 receives divide-by-two oscillator output signal OSC2, and generates divided oscillator output signal OSCD which has a predicted frequency of 12.5 MHz.

As further shown in FIG. 1, a range select counter 118 generates a first enable signal EN1 a preselected settling time after receiving a delayed reset signal RST and then, if range select counter 118 has not been reset,removes first enable signal EN1 and generates a second enable signal EN2 a preselected turn-off time after generating first enable signal EN1.

A phase error detector 120 compares divided oscillator output signal OSCD currently being generated by VCO 110 to a 12.5 MHz reference signal REF inresponse to first enable signal EN1. If a phase error is detected, then phase error detector 120 generates a shift signal, and then, after a delaytime, generates delayed reset signal RST. Phase error detector 120 suspendscomparison of divided oscillator output signal OSCD and reference signal REF when first enable signal EN1 is removed.

A shift register 122 selects a next operating range in response to shift signal SHF by generating a next range select signal from five range selectsignals RSS0-4.

A phase comparator 114 compares current divided oscillator output signal OSCD to reference signal REF and generates a difference signal DIF in response thereto.

A loop filter 116 responds to difference signal DIF by generating a corresponding loop filter voltage signal LFV for control of VCO 110.

When autoranging phase-lock-loop circuit 112 is energized, VCO 110 receivesa first range select signal RSS2 and a loop filter voltage LFV and in response generates a corresponding oscillator output signal OSC.

As stated above, phase comparator 114, receives divided oscillator output signal OSCD and the 12.5 MHz reference signal REF, compares the rising edges of divided oscillator signal OSCD and reference signal REF, and thenoutputs difference signal DIF which represents the difference between the frequency of divided oscillator signal OSCD and the frequency of referencesignal REF.

Loop filter 116 responds to difference signal DIF by either increasing or decreasing loop filter voltage LFV within the range of loop filter voltages capable of being generated by loop filter 116. In the preferred embodiment of the present invention, loop filter voltage LFV ranges from 1volt to 4 volts.

VCO 110 responds to the increased or decreased loop filter voltage LFV by increasing or decreasing, respectively, the frequency of oscillator outputsignal OSC until the frequency of divided oscillator output signal OSCD matches the 12.5 MHz frequency of reference signal REF.

VCO 110 is said to be "locked" to reference signal REF when both the phase and frequency of divided oscillator output signal OSCD and the phase and frequency of reference signal REF are matched within the error tolerance of autoranging phase-lock-loop circuit 112. On the other hand, VCO 110 is said to be "out of lock" when loop filter voltage LFV has been increased or decreased to the limits of loop filter 116, thereby increasing or decreasing the frequency of oscillator output signal OSC to its full extent, and the phase and frequency of divided oscillator output signal OSCD and the phase and frequency of reference signal REF remain unmatched.

In accordance with the present invention, if VCO 110 remains out of lock after a preselected settling time (see below), autoranging phase-lock-loopcircuit 112 commands VCO 110 to step to a new operating range by generatinga next range select signal RSS0-4. As discussed in greater detail below, the next operating range may have a center frequency which is greater thanor lesser than the center frequency of the present range.

By stepping from one operating range to another operating range with a constant loop filter voltage LFV, the frequency of oscillator output signal OSC changes by a 18.75 MHz step. This results in a frequency range of operation over the loop filter voltage range that is shifted up or downby 18.75 MHz from the original operating range.

When oscillator output signal OSC has been generated in the next operating range, autoranging phase-lock-loop circuit 112 attempts to lock oscillatoroutput signal OSC onto reference signal REF by again varying loop filter voltage LFV in response to difference signal DIF. If VCO 110 remains out of lock after the settling time has expired for a second time, then autoranging phase-lock-loop circuit 112 again commands VCO 110 to step to the next operating range by generating the next range select signal RSS0-4. This process is repeated as described above until VCO 110 locks onto reference signal REF. As stated above, in the preferred embodiment ofthe present invention, VCO 110 may operate in one of five operating ranges in response to one of five range select signals RSS0-RSS4.

FIG. 2 shows the five operating ranges FR0-FR4 as a function of loop filtervoltage LFV. As shown in FIG. 2, frequency range FR0 ranges from 175.00 to 250.00 MHz, frequency range FR1 ranges from 193.75 to 268.75 MHz, frequency range FR2 ranges from 212.50 to 287.50 MHz, frequency range FR3 ranges from 231.25 to 306.25 MHz, and frequency range FR4 ranges from 250.00 to 325.00 MHz.

Each of the five frequency ranges FR0-FR4 represents the range of frequencies wherein VCO 110 can lock on to a compatible reference signal. For example, if a 250 MHz reference signal REF is within second frequency range FR2, (212.50 MHz to 287.5 MHz), then VCO 110 will be able to lock onto reference signal REF by varying loop filter voltage LFV as described above.

If, however, reference signal REF is below second frequency range FR2; e.g., at 200 MHz, then VCO 110 will not be able to lock onto reference signal REF because loop filter voltage LFV will not have sufficient range;i.e., VCO 110 will bottom out at 212.5 MHz, and VCO 110 will remain out of lock after the settling time has expired. The autoranging phase-lock-loop circuit 112 will then step VCO 110 to a different operating range according to the particular search routine employed (as discussed in greater detail below).

Since the frequency of the next operating range is now 18.75 MHz lower thanthe original operating range (193.75 MHz to 268.75 MHz), VCO 110 will now be able to match the phase and frequency of reference signal REF by varying loop filter voltage LFV as noted above.

Referring again to FIG. 1, and as shown in STEP A of FIG. 3, autoranging phase-locked-loop circuit 112 generates a first command to operate in an operating range by generating a forced reset signal RSTF. Forced reset signal RSTF is generated approximately 6.6 mS (milliseconds) after autoranging phase-locked-loop circuit 112 has been powered up, reset by the hardware, or released from a test search routine (see below). The 6.6 mS delay is provided by a 6.6 mS timer circuit 412 (see FIGS. 4C and 4E).

As shown in FIG. 1 and STEP B of FIG. 3, shift register 122 receives forcedreset signal RSTF and in response generates second range select signal RSS2.

As shown in FIG. 1 and STEP C of FIG. 3, a ten-bit ripple range select counter 118 receives forced reset signal RSTF and, in response, removes a third enable signal EN3 (see below) and begins timing the settling time. Forced reset signal RSTF resets range select counter 118 a delay time after shift register 122 receives forced reset signal RSTF. The delay timeallows VCO 110 to begin generating an oscillator output signal OSC at substantially the same time that counter 118 begins timing.

The settling time, which in the preferred embodiment of the present invention is approximately 61.44 uS (microseconds) or 768 counts, is provided to allow VCO 110 sufficient time to lock onto reference signal REF by varying loop filter voltage LFV as described above. After the settling time has expired, as shown in STEP D of FIG. 3, range select counter 118 generates first enable signal EN1.

As shown in FIG. 1 and STEP E of FIG. 3, phase error detector 120, receivesfirst enable signal EN1, a divided oscillator output signal OSCD and reference signal REF and, in response, begins comparing the rising edges of divided oscillator output signal OSCD and reference signal REF to determine if a phase error is present. If divided oscillator output signalOSCD is out of phase from reference signal REF by more than +/-4 nanoseconds, a phase error exists. As shown in STEP F of FIG. 3, when a phase error exists, phase error detector 120 generates a shift signal SHF,which generates the next range select signal RSS0-4 by shifting shift register 122 in accordance with a selection routine (discussed below), andthen, after the delay time, generates a delayed reset signal RST, which resets counter 118 to begin counting again.

After second range select signal RSS2 has been generated following forced reset signal RSTF, shift register 122 selects the next operating range using one of two primary selection routines; a direct search routine or a barrel routine. Referring again to FIG. 1, the barrel routine, which includes a barrel up and a barrel down subroutine, is selected by asserting a BAR/DIR signal high. The direct search routine is selected by asserting the BAR/DIR signal low. The barrel up subroutine is selected by asserting a barrel up/barrel down signal UP/DN high; the barrel down subroutine is selected by asserting the barrel up/barrel down signal UP/DNlow.

When the barrel up subroutine has been selected, shift register 122 sequentially selects the oscillator output signal which has the next higher frequency. In the barrel up approach, each subsequent range select signal commands VCO 110 to increase the frequency of the current oscillator output signal by 18.75 MHz until the next 18.75 MHz increase would exceed 325.00 MHz. When the next increase would exceed 325.00 MHz, the next range select signal commands VCO 110 to reduce the frequency of the current oscillator output signal by 75 MHz (18.75 MHz times 4) whereupon subsequent range select signals command VCO 110 to again incrementally increase the frequency of the current oscillator output signal.

Conceptually, the barrel up approach may be thought of as sequentially stepping from frequency range FR2 to frequency range FR3 to frequency range FR4 to frequency range FR0 to frequency range FR1 to frequency rangeFR2.

Similarly, when the barrel down subroutine has been selected, shift register 122 continually selects the oscillator output signal which has the next lower frequency. In the barrel down approach, each subsequent range select signal commands VCO 110 to decrease the frequency of the current oscillator output signal by 18.75 MHz until the next 18.75 MHz decrease would fall below 175.00 MHz. When the next decrease would fall below 175.00 MHz, the next range select signal commands VCO 110 to increase the frequency of the current oscillator output signal by 75 MHz (18.75 MHz times 4) whereupon subsequent range select signals command VCO 110 to again incrementally decrease the frequency of the current oscillator output signal.

Conceptually, the barrel down approach may be thought of as sequentially stepping from frequency range FR2 to frequency range FR1 to frequency range FR0 to frequency range FR4 to frequency range FR3 to frequency rangeFR2.

If the direct selection routine has been selected, then shift register 122 receives the search up/search down signal SUP/SDN from filter voltage comparator 124. If filter voltage comparator 124 indicates that loop filter voltage LFV is in excess of 3.25 volts by asserting shift signal SHF, then shift register 122 selects the oscillator output signal which has the next lower frequency. If filter voltage comparator 124 indicates that loop filter voltage LFV is below 1.75 volts, then shift register 122 selects the oscillator output signal which has the next higher frequency.

As shown in FIG. 1, in addition to the above-described selection routines, autoranging phase-lock-loop circuit 112 also responds to a five-bit test signal TEST generated by a test circuit 414 (see FIGS. 4C and 4E) which commands shift register 122 to generate a particular range select signal thereby causing VCO 110 to step to a particular operating range.

As shown in STEP G of FIG. 3, if after a verification time has expired range select counter 118 has not been reset, range select counter 118 removes first enable signal EN1. The verification time, which in the preferred embodiment of the present invention is approximately 20.48 uS or256 counts, is provided to allow phase error detector 120 time to determinewhether oscillator output signal OCS has locked onto reference signal REF to within +/-195 ppm (parts per million). A +/-4 nanosecond phase difference during a 20.48 uS verification time period equates to a lock quality of +/-195 ppm.

Referring to FIGS. 4A and 4B, a first delay circuit 418 and a second delay circuit 420 are used to achieve the +/-4 nS phase error detection necessary in autoranging phase-lock-loop circuit 112. The first delay circuit 418 and the second delay circuit 420 receive a delay current whichis substantially independent of variations in temperature and supply voltage. The delay current is substantially independent of variations in temperature and supply voltage because the delay current is referenced to a bandgap voltage (see below).

The delay current is driven into a fixed base-emitter capacitor to obtain acontrolled first delay circuit 418 and second delay circuit 420. First delay circuit 418 and second delay circuit 420 are used to match both rising and falling edge transitions. Referring to FIG. 4D, a parallel pathmatching the CMOS gate delays is provided such that the delay delta betweenAIN and AOUT and AIN to ADLYOUT is the 4 nS delay. First delay circuit 418 and second delay circuit 420 are then connected to the autoranging phase-lock-loop circuit 112 (range select) by connecting CLK PH to AIN, DATA PH to BIN, PH CLK to AOUTDLY, and PH DATA to BOUT. This provides the controlled delay to phase error detector 120 in the autoranging phase-lock-loop circuit 112.

As shown in STEP H of FIG. 3, if first enable signal EN1 is removed prior to range select counter 118 being reset, range select counter 118 generates a second enable signal EN2 for one count.

Referring to FIG. 1, when range select counter 118 generates second enable signal EN2 for one count, filter voltage comparator 124 receives second enable signal EN2, loop filter voltage LFV, and a first reference voltage VREF1 and, in response, instantaneously compares the DC level of loop filter voltage LFV to first reference voltage VREF1. As shown in STEP I ofFIG. 3, filter voltage comparator 124 compares loop filter voltage LFV to first reference voltage VREF1 to determine if VCO 110 is locked onto reference signal REF near the end of the dynamic range of loop filter voltage LFV.

Referring again to FIG. 2, it can be seen that if loop filter voltage LFV is between 3.25 volts and 4 volts, an increase of loop filter voltage LFV by more than 0.75 volts due to temperature or power supply VCC fluctuations will cause VCO 110 to break lock. Similarly, if loop filter voltage LFV is between 1 volt and 1.75 volts, any decrease in loop filter voltage LFV which causes the voltage to be reduced by more than 0.75 voltswill cause VCO 110 to break lock.

As shown in STEP I of FIG. 3, when loop filter voltage LFV is between 1 volt and 1.75 volts or 3.25 volts and 4 volts, filter voltage comparator 124 will generate shift signal SHF and then, after the delay time, generate delayed reset signal RST. As described above, when delayed reset signal RST is generated, range select counter 118 is reset and begins timing the settling time. When shift signal SHF is generated, shift register 122 generates another range select signal in accordance with the selected search routine.

Filter voltage comparator 124 allows VCO 110 to lock onto reference signal REF in the middle of one of the frequency ranges so that minor excursions by loop filter voltage LFV will not cause oscillator output signal OSC to break lock.

As shown in STEP J of FIG. 3, when loop filter voltage LFV is between 1.75 and 3.25 volts, range select counter 118 generates a third enable signal EN3 and stops counting. At this point, VCO 110 has successfully locked onto reference signal REF in a frequency range that provides a sufficient dynamic range.

Referring again to FIG. 1, a triple pulse detector 126 is utilized to protect against a catastrophic failure of the loop. Triple pulse detector 126 receives third enable signal EN3 and, in response, begins detecting the presence of current oscillator output signal OSC and reference signal REF. As shown in STEP K of FIG. 3, if three or more rising edges of divided oscillator output signal OSCD occur without the occurrence of a rising edge of reference signal REF, then triple pulse detector 126 generates forced reset signal RSTF. Shift register 122 receives forced reset signal RSTF and in response generates second range select signal RSS2 again. Additionally, range select counter 118 receives delayed reset signal RST the delay time later, resets counter 118, disables third enablesignal EN3, and begins timing again.

Similarly, if three or more rising edges of reference signal REF occur without the occurrence of a rising edge of the oscillator output signal, triple pulse detector 126 will also generate delayed reset signal RST.

Additionally, triple pulse detector 126 and phase error detector 120 provide outputs from a test circuit. Once VCO 110 has locked onto reference signal REF, phase error detector 120 will continue to output shift signal SHF. Similarly, after lock, triple pulse detector 126 will generate shift signal SHF as described above. This capability allows benchtest equipment or automatic test equipment to capture shift signal SHF fromeither device and monitor quality-of-lock and loss-of-lock problems. Both of these problems are usually Sporadic events that automatic testers cannot locate by monitoring the current oscillator signal and the reference signal independently.

The phase error detector 120 will also provide a simple GO/NO GO digital test for lock, replacing the more cumbersome repetitive AC parametric testing presently in use. This represents both a faster, cheaper, and morereliable testing method.

Filter voltage comparator 124 also provides a test output. Once VCO 110 haslocked onto reference signal REF, filter voltage comparator 124 will continue to output shift signal SHF. By capturing shift signal SHF, automatic test equipment may track VCO gain versus frequency range performance. This allows better tracking of the device versus process and offers a new tool for yield analysis and enhancement. Being able to evaluate the critical relationship of VCO gain versus frequency range on an automated basis allows for more accurate data for future modeling.

In the preferred embodiment of the present invention, a portion of shift register 122, 6.6 millisecond timer circuit 412, test circuit 414, and a multiple active range detector 410 are configured as illustrated in FIG. 4C. Multiple active range detector 410 monitors range select signals RSS0-RSS4 and generates forced reset signal RSTF if more than one range select signal is active at a time. The 6.6 mS timer circuit 412 prevents forced reset signal RSTF from being issued until a 6.6 mS delay has expired after VCO 110 is powered up, reset in hardware, or released from atest search.

A portion of counter 118, phase error detector 120, and triple pulse detector 126 are configured as illustrated in FIG. 4D. The first delay circuit 418 and the second delay circuit 420 are configured as shown in FIGS. 4A and 4B. A portion of shift register 122, 6.6 millisecond timer circuit 412, test circuit 414, and a multiple active range detector 410 are configured as illustrated in FIG. 4E. A portion of counter 118, phase error detector 120, and shift register 122 are configured as illustrated in FIG. 4F.

Referring to FIG. 5, VCO 110 of the preferred embodiment is shown. As shownin FIG. 5, a VGS and VSW generation circuit 310, which is electrically coupled to three equivalent oscillator stages 318, 320, 322, generates a corresponding gate-to-source voltage VGS and a switch voltage VSW in response to range select signals RSS0-RSS4.

In addition, a unity-gain loop filter operational amplifier 324 receives loop filter voltage LFV, which is referenced to ground, and translates loop filter voltage LFV into a translated loop filter voltage LFVT, which is referenced to power supply VCC. Each of three oscillator stages 318, 320, 322, then receives gate-to-source voltage VGS, switch voltage VSW, and translated loop filter voltage LFVT and, in response, generates a corresponding oscillator signal P1-P3, respectively.

The three oscillator signals P1-P3 are equivalent except for a phase delay associated with each succeeding oscillator stage. As shown in FIG. 5, first oscillator signal P1, which is output from first oscillator stage 318, is input to second oscillator circuit 320. Since each of the three oscillator stages is equivalent, it can been seen that second oscillator signal P2, which is output from second oscillator stage 320, is equivalentto first oscillator signal P1 except for the time required for first oscillator signal P1 to be transformed by second oscillator stage 320 intosecond oscillator signal P2. Similarly, third oscillator signal P3 is equivalent to second oscillator signal P2 except for the time required forsecond oscillator signal P2 to be transformed by third oscillator stage 322into third oscillator signal P3.

FIG. 6 shows, one of three equivalent oscillator stages 318, 320, 322, configured as a differential pair 610. As shown in FIG. 6, differential pair 610 includes two legs 612 and 614 which alternately provide a currentpath for a fixed current ISW from a power supply VCC to a first current source 616. Each leg 612 and 614 of differential pair 610 includes a switching transistor 618a, 618b, respectively, having collectors 620a and 620b, respectively, connected first to a power supply VCC through resistors 624a and 624b, respectively and second to translated loop filtervoltage LFVT through varactors 626a and 626b, respectively, and having emitters 628a and 628b, respectively, connected to first current source 616.

The output voltage of each leg 62 and 614 of differential pair 610, which provides the oscillator output signal, is taken at collector terminals 620a and 620b of switching transistors 618a and 618b, respectively. The input of each leg 612 and 614, which, as stated above, is electrically coupled to the output of a previous oscillator stage, is at bases 630a and630b of each of switching transistors 618a and 618b, respectively.

In operation, the base-emitter junction of each switching transistor 618a, 618b, is alternately forward-biased and reverse-biased by oscillator output signal OSC and its compliment which have been provided by the previous oscillator stage so that one switching transistor 618a, 618b, turns on and off while the other switching transistor 618a, 618b, turns off and on, respectively.

As each switching transistor 618a, 618b, transitions from an off to an on state and from an on to an off state, the frequency of oscillator output signal OSC will be defined first by the voltage drop across its corresponding resistor, 624a, 624b, respectively, which is equivalent to the output voltage measured at collectors 620a and 620b of corresponding switching transistors 618a and 618b, respectively, and second by the slew rate.

The voltage drop across resistors 624a and 624b is a function of a peak voltage, i.e. the voltage drop across the resistor when the switching transistor is off or is non-conducting, and a low voltage, i.e. the voltage drop across the resistor when the switching transistor is on or conducting.

The slew rate is defined as the voltage swing divided by the time required for the switching transistors 618a and 618b to transition from the off to the on state or from the on to the off state while charging and discharging, respectively, varactors 626a and 626b.

Since, as stated above, the frequency of oscillator output signal OSC is a function of the voltage drop across resistors 624a and 624b and the slew rate, it therefore follows that the frequency of oscillator output signal OSC may be changed by changing either of these two parameters.

As stated above, each leg 612 and 614 of differential pair 610 alternately provides a current path for fixed current ISW. Since a constant current will be present whenever leg 612 or 614 is conducting, the frequency of the oscillator output signal may be changed by changing the resistance of resistors 624a and 624b because, in the presence of a constant current, the voltage drop varies with resistance.

To illustrate, if the voltage drop across resistors 624a and 624b is defined by a peak voltage of 5 volts and a low voltage of 4 volts and assuming, for the purposes of this example, that the slew rate is equivalent to 0.5 volts per nanosecond, then it would take 2 nanoseconds for the current oscillator signal to transition from a peak voltage to a low voltage. This is equivalent to 1 nanosecond per cycle or 500 MHz.

If the voltage drop across resistors 624a and 624b is changed so that the peak voltage remains at 5 volts but the low voltage is decreased to 3 volts, then it will take 4 nanoseconds for the current oscillator signal to transition from the peak voltage to the low voltage. This is equivalentto 4 nanoseconds per cycle or 250 MHz.

Thus, by reducing the voltage drop across resistors 624a and 624b, the frequency of the oscillator output signal OSC may be increased. Similarly,by increasing the voltage drop across resistors 624a and 624b, the frequency of oscillator output signal OSC may be decreased.

Referring to FIG. 7, which shows the preferred implementation of oscillatorstages 318, 320, and 322 of FIG. 5, resistors 624a and 624b are implementedutilizing first p-channel FETs (field effect transistor) P1 and P2, respectively. As is well known, field effect transistors, when properly biased, may operate in a linear or triode range where the field effect transistor behaves as a variable resistor. Thus, by properly biasing firstp-channel FETs P1 and P2, using five different bias voltages, five different resistor values and, therefore, five different voltage drops and, therefore, five different oscillator frequencies may be generated.

As shown in FIG. 7, first current source 616 is implemented as a first npn current source transistor Q50 having its collector connected to the emitters of switching transistors 618a and 618b, its base connected to a reference voltage VREF, and its emitter connected to ground through a first current source resistor R50.

As stated above, the frequency of oscillator output signal OSC may also be changed by changing the slew rate. Since the slew rate is defined as the amount of time required to discharge and charge varactors 626a and 626b, the slew rate may be defined by: ##EQU1##

Since, as stated above, fixed current ISW sourced by first current source transistor Q50 is constant, the slew rate may be changed by changing the capacitance on varactors 626a and 626b.

To illustrate, borrowing from the above example where the voltage drop across resistors 624a and 624b was defined by a peak voltage of 5 volts and a low voltage of 4 volts and the slew rate was 0.5 volts per nanosecond, further assume that the slew rate is defined by a current fromthe first current source of 4 milliampere and a capacitance of 0.8 picofarads. As stated above, it would take 2 nanoseconds to transition from the peak voltage of 5 volts to the low voltage of 4 volts. Now assumethat the capacitance is increased from 0.8 picofarads to 1.6 picofarads. The result is that the slew rate is 0.25 volts per nanosecond, translatingto a 250 MHz rate.

Thus, by increasing the capacitance, the frequency of oscillator output signal OSC may be decreased. Similarly, by decreasing the capacitance, thefrequency of oscillator output signal OSC may be increased.

Referring again to FIG. 6, the capacitance on varactors 626a and 626b is controlled by translated loop filter voltage LFVT. The translated loop filter voltage LFVT reverse-biases varactors 626a and 626b from 0.5 volts to 3.5 volts. Therefore, as stated earlier, the frequency of oscillator output signal OSC may be changed by varying loop filter voltage LFV.

Referring again to FIG. 7, in accordance with the preferred embodiment, varactors 626a and 626b are comprised of diode transistors Q12a and Q12b having collectors and bases connected to receive translated loop filter voltage LFVT and having emitters connected to collectors 620a and 620b of switching transistors 618a and 618b, respectively.

When switching transistor 618a, 618b in a particular leg is not conducting,the voltage on the emitter of diode transistor Q12a, , Q12b, , in that leg will rise to the peak voltage. Thus, if translated loop filter voltage LFVT is also high, the emitter-base junction of diode transistor Q12a, Q12b, will only be slightly reverse-biased. Similarly, if translated loop filter voltage LFVT is low in comparison to the voltage at the emitter of diode transistor Q12a, Q12b, the emitter-base junction will be strongly reverse-biased. The more diode transistors Q12a and Q12b are reversed-biased, the less internal capacitance is present on diode transistors Q12a and Q12b.

For example, when translated loop filter voltage LFVT is high, e.g., 4 volts, and the voltage at the emitter of diode transistor Q12a, Q12b, is also high, e.g., 4.3 volts, diode transistor Q12a, Q12b, is only slightly reversed-biased. On the other hand, when translated loop filter voltage LFVT is low, e.g., 1 volt, diode transistor Q12a, Q12b, is strongly reversed-biased. A full three volt voltage swing of loop filter voltage LFV, and therefore translated loop filter voltage LFVT, corresponds to a frequency variation of +/-12% from the center value. This is how the low-gain nature of VCO 110 of the preferred embodiment is achieved.

As further shown in FIG. 7, to guarantee a full voltage swing (an exact lowvoltage) regardless of any process variations between first p-channel FETs P1 and P2, npn clamping transistor Q14a and Q14b are utilized on each leg 612 and 614 of differential pair 610. Each clamping transistor Q14a, Q14b,is connected so that its collector is connected to power supply VCC, its base is connected to switch voltage VSW, and its emitter is connected to collectors 620a and 620b of the switching transistors 618a and 618b, respectively. The lowest voltage on the emitters of diode transistors Q12aand Q12b is equivalent to switching voltage VSW minus the voltage associated with the base-emitter junction of clamping transistors Q14a andQ14b. This is necessarily so because once the voltage drops below this value, clamping transistors Q14a and Q14b become forward-biased and begin to source current.

The clamping transistors Q14a and Q14b guarantee that a full voltage swing will be realized by allowing the gate-to-source voltage of first p-channelFETs P1 and P2 to be set so that first p-channel FETs P1 and P2 will sourcea current approximately 10% less than the current demanded by fixed currentISW. Thus, as first current source transistor Q50 attempts to sink fixed current ISW from first p-channel FETs P1 and P2, the voltage at collectors620a and 620b of the switching transistors 618a and 618b, respectively, will drop and clamping transistors Q14a and Q14b, respectively, will become forward-biased, turning on to supply the remaining current to firstcurrent source transistor Q50.

For example, assume that the desired source-to-drain voltage is 0.3 volts and further assume that the resistance required to achieve the 0.3 source-to-drain voltage is 1500 ohms. In this situation, in order for clamping transistor Q14a, Q14b, to turn on, the resistance of first p-channel FETs P1 and P2 is set to, for example, 1700 ohms. By setting theactual resistance slightly higher than the resistance needed, the designer can be assured that, even with process variations, a full voltage swing isachieved.

As shown in FIG. 7, sources 730a and 730b of the first p-channel FETs P1 and P2, respectively, are connected to a voltage shifter transistor 732 configured as a diode. Voltage shifter transistor 732 allows the lower voltage swing level, as referenced to power supply VCC, to be equivalent to switching voltage VSW plus the voltage drop associated with the base-emitter junctions of voltage shifter transistor 732 and clamping transistor Q14a, Q14b, so that clamping transistor Q14a, Q14b, will be able to turn on.

Schematic diagrams of a portion of oscillator stages 318, 320, and 322 of the preferred embodiment are shown in FIGS. 8A, 8B, 8C, and 8D. In addition, a bias circuit 810 for the emitter-follower output stage of oscillator stages 318, 320, 322 are shown in FIG. 8B. Further, a partial start-up circuit 812, which keeps VCO 110 deenergized until power supply VCC has reached approximately 4 volts, is shown in FIG. 8C.

As stated above, by properly biasing first p-channel FETs P1 and P2, five different resistor values and, therefore, five different voltage drops and, therefore, five different oscillator frequencies may be generated. The first p-channel FETs P1 and P2 are biased by controlling the source-to-drain voltage VSD and the gate-to-source voltage VGS. The source-to-drain voltage VSD and the gate-to-source voltage VGS are controlled by VGS and VSW generator circuit 310.

FIG. 9 shows VGS and VSW generator circuit 310 of the preferred embodiment.As shown in FIG. 9, the gate of a second p-channel FET Q20 is connected to the gates of first FETs P1 and P2 through a VGS translator circuit 822. Inaddition, the drain of second FET Q20 is connected to the drain of first FETs P1 and P2 through an operational amplifier 816 and a VSW translator circuit 836.

Thus, at 40 degrees celsius, the gate-to-source voltage, the source-to-drain voltage, and a second current ISW2, which is pulled through second FET Q20 when a delta temperature current ISWD4 is equal to zero (see below), are equivalent to the gate-to-source voltage, the source-to-drain voltage, and fixed current ISW, which is pulled through first FETs P1 and P2 when delta temperature current ISWD4 is equal to zero. Therefore, by setting the gate-to-source voltage, the source-to-drain voltage, and second current ISW2 of second FET Q20, the gate-to-source voltage, the source-to-drain voltage, and fixed current ISWof first FETs P1 and P2 will also be set.

The source-to-drain voltage across second FET Q20 is set by switch voltage VSW and the operation of operational amplifier 816. Switch voltage VSW is equivalent to the voltage drop across one of five oscillator select transistors TP1-TP5 and its corresponding switch resistor R1-R5.

Each oscillator select transistor TP1-TP5 , having a source connected to internal power supply VCCI, having a drain connected to its corresponding switch resistor R1-R5, and having a gate connected to shift register 122 (see FIG. 1), provides a current path for a third current ISW3 when one ofthe oscillator select transistors TP1-TP5 is selected.

Third current ISW3 is generated by a third npn current source transistor Q24, which is matched to first current source transistor Q50, having a collector connected to each switching resistor R1-R5, having a base connected to reference voltage VREF, and having an emitter connected to ground through a third current resistor R6.

In operation, one of the five range select signals RSS0-RSS4 turns on a corresponding oscillator select transistor TP1-TP5 , thereby producing a current path for third current ISW3 and a voltage drop across the oscillator select transistor TP1-TP5 and its associated switch resistor R1-R5.

Operational amplifier 816, having a non-inverting input connected to switching voltage VSW and having an inverting input connected to the drainof second FET Q20, forces the source-to-drain voltage of second FET Q20 to assume the switching voltage VSW by the feedback operation of operational amplifier 816.

By forcing the source-to-drain voltage to be equivalent to switching voltage VSW, switching voltage VSW is equivalent to the source-to-drain voltage VSD across second FET Q20.

The gate-to-source voltage across second FET Q20, having a source connectedto internal power supply VCCI, having a drain connected to the inverting input of an operational amplifier 816 and a collector of a second current source transistor Q22, and having a gate connected to the output of an operational amplifier 816 and a gate-source translator circuit 822, is setby a second current ISW2 and the operation of operational amplifier 816.

A second npn current source transistor Q22, having a collector connected tothe drain of second FET Q20, having a base connected to a reference voltageVREF, and having an emitter connected to ground through a second current resistor R7, sources second current ISW2 which is substantially equivalentto 90% of fixed current ISW sourced by first current source transistor Q50.

Operational amplifier 816 forces the gate-to-source voltage to a voltage which will provide second current ISW2 at a source-to-drain voltage which is equivalent to switching voltage VSW.

VGS and VSW generator circuit 310 may utilize an internal power supply VCCIof approximately 3 volts, which is different from power supply VCC, to reduce power supply noise coupling into operational amplifier 816. The VGStranslator circuit 822 and the VSW translator circuit 836 are provided to translate back from the internal power supply VCCI referenced levels to levels referenced to the power supply VCC, which are what are required by VCO 110.

VGS and VSW generator circuit 310 of the preferred embodiment is shown in FIG. 10.

The above description describes the operation of the VCO at +40 degrees celsius. As temperature varies, however, the slew rate and therefore the frequency of oscillator output signal OSC, will also vary due to a linear change in the capacitance of all the transistors. As temperature increasesand decreases, the capacitance of varactors Q12a and Q12b increases and decreases, respectively. As the capacitance increases and decreases, the switching speed of oscillator stages 318, 320, and 322 decreases and increases. To maintain a constant switching speed, the current flowing through the switching transistors must be increased or decreased dependingon the temperature shift.

Thus, to achieve a nearly constant slew rate over changes in the surrounding temperature from -55 degrees celsius to +125 degrees celsius, the fixed, second, and third currents ISW, ISW2, and ISW3 are made to be substantially independent of the surrounding temperature and a delta temperature current is generated so that more or less current can be pulled through the switching transistor 618a, 618b when the capacitance increases and decreases, respectively.

Referring again to FIG. 5, VCO 110 of the preferred embodiment generates the fixed, second, and third currents ISW, ISW2, and ISW3 to be substantially independent of changes in the surrounding temperature by utilizing a voltage translator circuit 316 to generate reference voltage VREF which in turn generates the fixed, second, and third currents ISW, ISW2, and ISW3. In addition, voltage translator circuit 316 generates a temperature independent current IREF which is substantially temperature-independent, depending only on the P+ sheet rho.

Voltage translator circuit 316 generates voltage reference signal VREF in response to a temperature independent voltage of 1.35 volts and changes inthe surrounding temperature. The voltage reference signal VREF is generatedso that as the surrounding temperature rises and falls, voltage reference signal VREF decreases and increases, respectively, by a compensating amount so that the fixed, second, and third currents ISW, ISW2, and ISW3 may be constant.

The fixed, second, and third currents ISW, ISW2, and ISW3, however, remain dependent on the linear variation of the P+ sheet rho (90 ohm/sq). Since this dependency is small, the fixed, second, and third currents ISW, ISW2,and ISW3, to a first order, are independent of changes in the surrounding temperature.

Referring to FIG. 11, VCO of the preferred embodiment pulls more or less current through switching transistors 618a and 618b when the capacitance increases and decreases, respectively, by utilizing a temperature compensation circuit 314.

The temperature compensation circuit 314 includes an input stage 1102 that receives a temperature independent and dependent voltage, a temperature dependent stage 1104 for generating the temperature dependent voltage, a discharging stage 1106 for varying a discharge current Id as the surrounding temperature changes, and an output stage 1108 for generating adelta temperature current Iswd.

As shown in FIG. 11, in the preferred embodiment, input stage 1102 is configured as a compensating differential pair 1118. Compensating differential pair 1118 includes a charging leg 1120 and a discharging leg 1122, each of which provides a current path for a portion of a fixed current 0.17ISW from a power supply VCC to a charging current source transistor Q60.

Charging leg 1120 includes a p-channel charging transistor Q3, having a source connected to power supply VCC, and a npn charging input transistor Q4, having a collector connected to the gate and drain of charging transistor Q3, having a base connected to a temperature independent bandgap voltage VREF1 of approximately 2.5 volts, and having an emitter connected to the collector of charging current source transistor Q60 through a charging input resistor R1.

Discharging leg 1118 includes a p-channel discharging transistor Q5, havinga source connected to power supply VCC, and a discharging input transistor Q6, having a collector connected to the gate and drain of discharging transistor Q5, having a base connected to a temperature dependent node B, and having an emitter connected to the collector of charging current source transistor Q60 through a discharging input resistor R2.

Charging current source transistor Q60, having its base connected to the reference voltage VREF and having its emitter connected to ground through charging resistor R60, generates fixed current 0.17ISW, which is substantially temperature-independent, to be approximately 17% of fixed current ISW by increasing the value of the charging resistor R60 in relation to resistor R50 of FIG. 7.

As shown in FIG. 11, when charging input transistor Q4 has approximately 2.5 volts at its base and discharging input transistor Q6 has approximately 2.5 volts at its base, charging input transistor Q4 along with charging transistor Q3 and discharging input transistor Q6 along withdischarging transistor Q5, source approximately an equivalent portion of the fixed current 0.17ISW.

On the other hand, as the temperature changes, the voltage on the base of discharging input transistor Q6 changes, thereby changing the proportion of the fixed current 0.17ISW which is sourced by charging input transistorQ4 and discharging input transistor Q6.

Temperature dependent stage 1104 varies the voltage at temperature dependent node B and the base of discharging input transistor Q6 as temperature varies. Temperature dependent node B is connected to ground through a series connection of a dependent resistor R3, a first diode D1, and a second diode D2, and to power supply VCC through an independent current source 1138. Independent current source 1138 sources temperature dependent current IREF which is derived from voltage translator circuit 316.

As temperature varies, the voltage drop across first diode D1 and second diode D2 will vary causing the voltage at temperature dependent node B andthe base of discharging input transistor Q6 to vary. As the voltage at the base of discharging input transistor Q6 varies, the proportion of the fixed current 0.17ISW sourced by charging input transistor Q4 and discharging input transistor Q6 changes. Thus, as the temperature changes,the portion of the fixed current 0.17ISW sourced by charging input transistor Q4 and discharging input transistor Q6 changes.

Output stage 1108 generates delta temperature current ISWD as a summation of a charging current Ic and the discharging current Id. The charging current Ic is generated by a p-channel charging output transistor Q1.

Charging output transistor Q1, having a source connected to power supply VCC, having a gate connected to the gate and the drain of charging transistor Q3, and having a drain connected to a delta temperature node A,generates charging current Ic by connecting its gate to the gate of charging transistor Q3.

By connecting gates together, charging transistor Q3 and charging output transistor Q1 have substantially equivalent gate-to-source voltages. Thus,when the source-to-drain voltage of charging transistor Q3 becomes positiveand charging transistor Q3 begins to conduct, charging output transistor Q1will also begin to conduct.

N-channel discharging output transistor Q2, having a drain connected to delta temperature node A and having a source connected to ground, generates discharge current Id by mirroring an intermediate current Im.

Intermediate current Im is generated by the discharging stage. A p-channel conversion transistor Q7, having a source connected to the power supply VCC, having a gate connected to the gate and drain of discharging transistor Q5, generates intermediate current Im by connecting its gate tothe gate of discharging transistor Q5.

By connecting gates together, discharging transistor Q5 and conversion transistor Q7 have substantially equivalent gate-to-source voltages. Thus,when the source-to-drain voltage of discharging transistor Q5 becomes positive and discharging transistor Q5 begins to conduct, conversion transistor Q7 will also begin to conduct.

A n-channel output transistor QS, whose drain and gate are connected to thedrain of conversion transistor Q7 and the gate of discharging output transistor Q2, and whose source is connected to ground, conducts intermediate current Im.

Discharging output transistor Q2 generates discharge current Id by connecting its gate to the gate of output transistor QS. By connecting gates together, output transistor Q8 and discharging output transistor Q2 have substantially equivalent gate-to-source voltages. Thus, when the source-to-drain voltage of output transistor Q3 becomes positive and the output transistor Q3 begins to conduct, the discharging output transistor Q2 will also begin to conduct.

In operation, at +40 degree celsius, the charging output transistor Q1 sources a charging current Ic which is identical to discharging current Idwhich is sourced by discharging output transistor Q2. Thus, at +40 degrees celsius, discharging output transistor Q2 sinks all of the current generated by charging output transistor Q1.

As temperature changes, however, compensating differential pair 1118 indirectly causes charging output transistor Q1 and discharging output transistor Q2 to source different amounts of charging current Ic and discharging current Id, respectively. When discharging current Id is less than charging current Ic, delta temperature node A effectively sources a delta temperature current Iswd which is equivalent to the difference between charging current Ic and discharging current Id.

Similarly, when discharging current Id is greater than charging current Ic,delta temperature node A effectively sinks a delta temperature current Iswdcurrent by drawing the needed current from VGS and VSW generator circuit 310 and each oscillator circuit 318, 320, 322.

In the preferred embodiment, four output stages are electrically connected in parallel to produce four equivalent delta temperature currents ISWD1-4 (see FIG. 5).

The fixed current 0.17ISW is selected to be approximately 17% of the nearlyconstant fixed current ISW. In order to accurately compensate for the variation in capacitance with temperature over the range -55 degrees celsius to +125 degrees celsius centered around +40 degrees celsius, it was determined that the temperature compensation circuit 314 should implement the equation ##EQU2##

A portion of voltage translator circuit 316 and the temperature compensation circuit 314 of the preferred embodiment of the present invention are shown in FIGS. 12A, 12B, 12C, and 12D.

Referring again to FIG. 7, as stated above, first Current source transistorQ50 sinks a fixed current ISW through switching transistors 618a and 618b independent of temperature. As temperature and therefore capacitance rises, the delta temperature current sinks an additional current which, when combined with the fixed current ISW, forms a larger first current ISW1. This larger current is sufficient to compensate for the larger capacitance and thereby maintains a constant slew rate. Referring to the equation ##EQU3##if C increases with temperature in a linear manner, then in order to keep dv/dt constant, ISW1 must also increase in the same linear manner with temperature.

By sinking first current ISW1 through switching transistors 618a and 618b, a potentially greater source-to-drain voltage drop could be created acrossfirst p-channel FETs P1 and P2. However, referring to FIG. 9, the product of third current ISW3 and the selected switch resistor R1-R5 is substantially independent of temperature. This sets the switching voltage to be substantially independent of temperature and therefore, due to the feedback operation of operational amplifier 816, sets the source-to-drain voltage to be substantially independent of temperature.

As stated above, second current ISW2, which is also substantially independent of temperature, sets the gate-to-source voltage of second p-channel FET Q20. As temperature rises, delta temperature current ISWD sinks an identical additional current which, when combined with second current ISW2, forms a larger fifth current ISW5.

By pulling a larger fifth current ISW5 through second FET Q20, the feedbackaction of the operational amplifier changes the gate-to-source voltage of second FET Q20. As stated above, this then changes the gate-to-source voltage of first FETs P1 and P2 so that the voltage drop across first FETsP1 and P2 remains constant with the increased first current ISW1 being pulled through first FETs P1 and P2.

Similarly, as the temperature decreases, delta temperature current ISWD sources an additional current resulting in first current ISW1 and fifth current ISW5 being reduced.

The autoranging phase-lock-loop of the present invention has several advantages. First, the autoranging phase-lock-loop allows the VCO 110 to self determine its optimal range of operation, and then program itself without factory or user intervention. Upon powerup, the device makes a series of measurements that determine the optimal range of operation. Oncethe device is locked on a specific range of operation, then the low-gain VCO 110 is able to lock to and track any variations in the incoming reference signal as the environment varies over temperature and supply voltage.

The autoranging phase-lock-loop 112 also allows circuit implementation using the cheapest, simplest fabrication process available, as well as keeping both the testing, and use of the device as simple as possible.

It should be understood that various alternatives to the structures described herein may be employed in practicing the present invention. It is intended that the following claims define the invention and that the structure within the scope of these claims and their equivalents be covered thereby. 

What is claimed is:
 1. An autoranging phase-lock-loop circuit for locking the output of a voltage controlled oscillator onto a reference frequency, the autoranging phase-lock-loop circuit comprising:range programmable voltage controlled oscillator means for generating a current oscillator output signal in response to one of a plurality of range select signals, each range select signal corresponding to a range of oscillator output frequencies, and for varying a frequency of the current oscillator output signal in response to a loop filter voltage; counter means for generating a first enable signal a preselected settling time after receiving a reset signal, for removing the first enable signal a preselected turn-off time after generating the first enable signal if the counter means has not received a subsequent reset signal since a most recent first enable signal was generated, and for generating a second enable signal after removing the first enable signal; phase error detector means for comparing the current oscillator output signal to a reference signal in response to the first enable signal, for generating a shift signal and the reset signal if a phase error is detected, the reset signal being generated a delay time after the shift signal, and for suspending a comparison of the current oscillator output signal to the reference signal when the first enable signal is removed; shift register means for selecting a next range of oscillator output frequencies in response to the shift signal by generating a new range select signal from the plurality of range select signals; phase comparator means for comparing the current oscillator output signal to the reference signal and for generating a difference signal in response thereto; and loop filter means for generating the loop filter voltage in response to the difference signal.
 2. The autoranging phase-lock-loop circuit of claim 1 further comprising filter voltage comparator means for comparing the loop filter voltage to a high reference voltage and a low reference voltage in response to the second enable signal and for generating the shift signal and the reset signal if the loop filter voltage exceeds the high reference voltage or falls below the low reference voltage.
 3. The autoranging phase-lock-loop circuit of claim 2 wherein the counter means removes the second enable signal a measurement time after generating the second enable signal if the counter means has not received a subsequent reset signal since a most recent second enable signal was generated and generates a third enable signal after removing the second enable signal.
 4. The autoranging phase-lock-loop circuit of claim 3 wherein the counter stops counting after the third enable signal has been generated.
 5. The autoranging phase-lock-loop circuit of claim 4 and further comprising a triple pulse detector for comparing the current oscillator output signal and the reference signal in response to the third enable signal and for generating the shift signal and the reset signal if the current oscillator output signal or the reference signal is not present for a failure time.
 6. The autoranging phase-lock-loop circuit of claim 5 wherein the means for selecting the next range of oscillator output frequencies further comprises:barrel up means for sequentially selecting, in response to each subsequent shift signal, an operating range having a next higher center frequency until an operating range having a highest center frequency has been selected at which time an operating range having a lowest center frequency is selected; barrel down means for sequentially selecting, in response to each subsequent shift signal, an operating range having a next lower center frequency until the operating range having the lowest center frequency has been selected at which time the operating range having the highest center frequency is selected; and direct selection means for selecting a specific operating range. 